NUMERICAL SOLUTION OF LONGITUDINAL AND TORSIONAL OSCILLATIONS OF A CIRCULAR CYLINDER WITH SUCTION IN A COUPLE STRESS FLUID
|
|
- Walter Parsons
- 5 years ago
- Views:
Transcription
1 VOL. 5, NO. 5, MAY IN ARPN Jounal of Engneeng and Appled cence 6- Aan Reeac Publng Neok (ARPN). All g eeed..apnjounal.com NUMERICAL OLUTION OF LONGITUDINAL AND TORIONAL OCILLATION OF A CIRCULAR CYLINDER WITH UCTION IN A COUPLE TRE FLUID J. V. Ramana Muy, G. Nagaaju and P. Muu Depamen of Maemac, Naonal Inue of Tecnology, Waangal, A.P., Inda E-Mal: jjoyula@yaoo.co.n ABTRACT Te flo of a couple e flud geneaed by pefomng longudnal and oonal ocllaon of a poou ccula cylnde ubjeced o conan ucon a e uface of e cylnde uded. A fne dffeence meod popoed o analyze e elocy componen, n an nfne expane of an ncompeble couple e flud unde anng couple ee of ype A condon o upe adeence condon of ype B on e bounday. Te effec of couple e paamee, Reynold numbe and e ao of couple e coe paamee on anee and axal elocy componen ae uded. Te dag foce acng on e all of e cylnde deed and effec of couple e paamee on dag ae on gapcally. Keyod: couple e flud, longudnal and oonal ocllaon, dag, ucon, njecon.. INTRODUCTION In numeou ecnologcal applcaon, e flud n ue do no obey e commonly aumed lnea elaonp beeen e e and e ae of an a a pon and e accuae flo beao canno be pedced by e clacal Neonan eoy. uc flud ae ecognzed a non-neonan flud. In pacula, e nee n non-neonan flud a gon condeably, due lagely o e demand of uc dee aea a boeology, geopyc and cemcal and peoleum ndue. Fo eaon eeal model ae been popoed o pedc e non-neonan beao of aou ype of flud. One cla of flud c a ganed condeable aenon n ecen yea e couple e flud. Couple ee ae a conequence of e aumpon a e neacon of one pa of a body on anoe, aco a uface, equalen o a foce and momen dbuon. Couple e flud con of gd, andomly oened pacle upended n a cou medum uc a blood flud, eleco-eologcal flud and ynec flud. Te man feaue of couple e flud a e e eno an-ymmec. oke [] genealzed e clacal model o nclude e effec of e peence of e couple ee and couple e model a been dely ued becaue of elae Maemacal mplcy compaed e oe model deeloped fo effec of e couple ee. T flud eoy dcued n deal by oke melf n eae Teoe of Flud Mcoucue [] een e alo peened a long l of poblem dcued by eeace efeence o eoy. Recenly, e udy of couple e flud flo a been e ubjec of gea nee, due o depead ndual and cenfc applcaon n pumpng flud, uc a ynec flud, polyme-ckened ol, lqud cyal and anmal blood. Oe mpoan feld ee couple e flud ae applcaon ae queezng and lubcaon eoy. Te moon of flud oug poou pemeable uface a lo Reynold numbe a long been an mpoan ubjec n e feld of cemcal, bomedcal, and enonmenal engneeng and cence. T penomenon fundamenal n naue and of gea paccal mpoance n many dee applcaon lke poducon of ol and ga fom geologcal ucue, e gafcaon of coal, e eong of ale ol, flaon, uface caaly of cemcal eacon, adopon, coalecence, dyng, on excange and comaogapy. ang fom Couee flo, e flo geneaed n flud by e moon of uface ae been aacng e eeace. Among em, e udy of flo due o longudnal and oonal ocllaon peen ome nee n dffeen engneeng aea lke Oceanogapy, e ecnology of baon on macney, e poce of cean polyme lqud cyal, and e offoe dllng of ol. Tee ae ee pycal uaon n c e udy of e longudnal and oonal ocllaon can be appled. Te f applcaon n lubcaon eoy. Te cylndcal beang conanng a non-neonan flud lubcan ae ubjec o longudnal and oonal baon on e macney. A econd applcaon e flo of polyme lqud cyal made of dumbbell lke molecule poceed nde a ccula cylnde c ubjec o longudnal and oonal ocllaon. And fnally, a poble d applcaon e flo of mud n e dllng of an offoe ol dllng un c ubjeced o ocllaon due o oceanc ae. Te moon of a clacal cou flud due o e oaon of an nfne cylndcal od mmeed n e flud a f decbed by oke []. Lae follong e ok, many flo poblem due o e moon of bode ee oled. ome flo poblem elaed o e moon of a cylndcal od pefomng longudnal and oonal ocllaon ae gen belo. Caaella e al., [] uded e exenal flo due o longudnal and oonal ocllaon of a od n a Neonan flud and obaned an exac oluon fo e ame. Rajagopal [5] uded e 5
2 VOL. 5, NO. 5, MAY IN ARPN Jounal of Engneeng and Appled cence 6- Aan Reeac Publng Neok (ARPN). All g eeed..apnjounal.com ame poblem fo e cae of a econd gade flud. Ramkoon and Majumda [6] uded e nenal flo due o longudnal and oonal ocllaon of a cou flud and ey deed an analycal expeon fo eloce, ea ee and dag on e cylnde. Ramkoon e al., [7] obaned an exac oluon fo an nfne od undegong bo longudnal and oonal ocllaon n a pola flud and ey ae peened e effec of mcopola paamee on e mcooaon and elocy feld gapcally. Calmele-Eluu e al., [8] uded e nenal flo of a mcopola flud nde a ccula cylnde ubjec o longudnal and oonal ocllaon and ey ae on e effec of mcopola flud on o componen elocy feld oug gap. Oen and Raaman [9] uded e ame ype of flo an Oldoyd-B lqud. A lage numbe of eoecal negaon dealng eady ncompeble lamna flo ee njecon o ucon a e boundae ae appeaed dung e la fe decade. eeal auo, o menon ome [-] ae uded e eady lamna flo of an ncompeble cou flud n a o-dmenonal cannel paallel poou all. oundalgeka e al., [] uded e effec of couple ee on e ocllaoy flo pa poou, nfne, fla plae en e fee eam elocy ocllae n magnude abou a conan mean. Eldabe e al., [5] ae uded e effec of couple ee on an uneady MHD Eyng Poell model of non-neonan flud flo beeen o paallel fxed poou plae unde a unfom exenal magnec feld. Tey ae on e effec of couple e paamee and Hamann numbe on elocy dbuon oug gap. Deaka e al., [6] uded e oke f and econd poblem fo an ncompeble couple e flud by ung e condon a couple ee an on e bounday. Tey ae ploed e elocy pofle fo dffeen me and dffeen alue of couple e Reynold numbe. naacaya e al., [7] uded e lamna flo of a couple e flud n a poou cannel expandng o conacng all ymmec njecon o ucon along e unfomly expandng poou all by ung mlay anfomaon. Tey ae peened gap fo elocy componen and empeaue dbuon fo dffeen alue of e flud and geomec popee. Ramana Muy e al., [8] uded e eady MHD flo of a mcopola flud oug a poou ccula ppe conan ucon/njecon. Tey ae on e effec of kn fcon epec o mcopola paamee and Hamann numbe oug gap. To e exen of e knoledge of e auo, ey fe leaue ae aalable on e flo due o ocllaon of a od n couple e flud. Te poblem menoned n [7] and [8] ae ome example n decon. Hence, n pape e conde e flo of couple e flud geneaed by a poou ccula cylnde pefomng longudnal and oonal ocllaon and ubjeced o ucon elocy a e uface.. FORMULATION OF THE PROBLEM Conde a poou ccula cylnde of adu a n an nfne expanon of a couple e flud. Te cylnde ubjeced o oonal ocllaon, Exp (ω ) and longudnal ocllaon, Exp (ω ) amplude q nβ, q co β along e epece decon ee ω e fequency of e oonal ocllaon, ω e fequency of e longudnal ocllaon, q e magnude of e ocllaon and β e angle beeen e decon of oonal ocllaon and e bae eco e θ..e., e cylnde ocllae elocy a gen by e expeon ( ωτ ωτ Q q n β e e Co β e e ) Γ θ u a ucon o njecon elocy on e uface of e poou cylnde. Cylndcal pola coodnae yem condeed e Z-ax along e ax of e cylnde and ogn on e ax. Le R, θ and Z denoe e adal, azmual and axal coodnae epecely of a pon n e egon of flo. No e conde e flo geneaed n e couple e flud due o e ocllaon of e cylnde. Te pycal model lluang e poblem unde condeaon on n Fgue-. Fgue-. Geomecal epeenaon of e poblem: non-dmenonal fom. Afe neglecng body foce and body couple, e condon of ncompebly and e equaon moon fo a couple e flud, a gen by oke [] ae: Q () Q ρ Q Q P µ Q τ η Q () Wee Q elocy eco, P flud peue, z. ρ deny, τ me, µ coy and η couple e coy coeffcen, e dmenonal gaden. By 5
3 VOL. 5, NO. 5, MAY IN ARPN Jounal of Engneeng and Appled cence 6- Aan Reeac Publng Neok (ARPN). All g eeed..apnjounal.com naue of e flo, e elocy componen ae axally ymmec and depend only on adal dance and me. Hence e elocy eco aken of e fom ( R) e V ( R,τ) eθ W ( R,τ) e z Q U () Le u noduce e follong non dmenonal ceme ωa ω σ, σ a R,, Q P q, p, q q a q ρ q q u U V τ, n, u,, W () a q q q q By e non-dmenonal ceme () n () and (), e equaon fo e flo ae anfomed o e follong non-dmenonal fom.. q (5) q Re q. q Re p q q (6) ρq ee Re a η Reynold numbe and µ µ a couple e paamee. No o mac e ocllang bounday, e elocy n () aumed n e fom σ σ () e () e eθ ( ) e ez q u (7) Te equaon (6) ll ge ae o e follong ee cala equaon n e decon of bae eco dp n d σ e (8) n Re σ D D n Re σ ee (9) and D D Ung D and D n e equaon (9), e ge a () a a ee Re n a, a, a Re σ and Ren a a mlaly e e () a () b b b () ee Ren b, b Reσ and b No e equaon () and () ae oled fo and unde e no lp condon and ype A condon o ype B condon on e bounday. Tee condon ae gen a follo.. BOUNDARY CONDITION No lp condon Te elocy of e flud on e bounday equal o e elocy of e bounday. I explcly gen by Q Velocy of Γ Γ q ω τ ω τ ( coβ e n β e e ) eθ I ake e follong n non-dmenonal fom σ q co β e e θ n β e T condon can be explcly en a n e follong equaon coβ nβ () ( ) And ( ) Type A condon Type A-condon epeen anng of couple e eno on e bounday. Te conue equaon fo couple e eno M gen by M mi η ( Q ) η [ ( Q ] T ) () Takng equaon (), e ge e expeon fo M a M m e e e e e e σ σ q e e θ e e z ( ) θ θ z z η q η q σ e e e θ a η q a a η q a e σ z e z σ e θe n e 5
4 VOL. 5, NO. 5, MAY IN ARPN Jounal of Engneeng and Appled cence 6- Aan Reeac Publng Neok (ARPN). All g eeed..apnjounal.com η q σ η q σ D e e e z D e e ze a a If M ane on e bounday, e ge e condon a D and e ee e η η on (5) Type B condon Type B-condon e upe adeence condon on e bounday. T condon eque a angula elocy of e flud pacle on e bounday equal o angula elocy of e bounday..e., ω Γ QΓ mple a d σ And ( ) d (6) A, e flud a e and bounday condon can be aken a D e d d ( ) on (7). FINITE DIFFERENCE METHOD OF OLUTION In e of e complcaed naue of o equaon () and (), e analycal oluon fo and eem o be beyond eac. Te deal of fne dffeence meod ued ee can be uded fom Ref. [9], fo obanng e oluon fo and. We ake 5 un of dance fom ogn ey lage epeenng nfny. Hence e dcee e neal [, 5] no n ubneal n node. Eac node epeened by, 9/n e ep leng, ang fom f node o e la node n 5. Te alue of e funcon, a ae gen by and. Te ymmec deae fomulae a e node ae gen a belo: 6 (8) ubung ee deae gen n (8), n e equaon () e ge,,,, 5, (9) ee, ( ), a ( ) ( ) a, 6 a ( a ) a ( ), a ( ) a () 5, Te fne dffeence fom of () a e follong:,,,, 5, (), ( ), b ( ) ( b ) b b, 6 ( ), b ( b ) () 5, Type A oluon fo eloce and We ake e follong bounday condon ( ) coβ n D, n, and D () Ealuang (9) fo dffeen alue of e oban : : :,,, 5,,,,, 5,, 5
5 VOL. 5, NO. 5, MAY IN ARPN Jounal of Engneeng and Appled cence 6- Aan Reeac Publng Neok (ARPN). All g eeed..apnjounal.com,,, 5,, :,,,, 5, 5 n :, n n,n n,n n 5,n n, n n n:, n n,n n,n n 5,n n,n n () Tu e yem of equaon () epeen n equaon n n unknon. Hence e eque o moe equaon. Tee can be obaned fom D And D (5) Ung e bounday condon (5), en e ae and n 5 n 6 n (6) Wee,,, n n n, 5 n and 6 n Expeng e equaon () and (6) n max fom a A X B (7) ee e mace A, X and B ae gen n e appendx. B conan and n c ae e alue of on e bounday and X con of alue of n e egon. olng e yem (7) e ge e oluon fo. No e fnd oluon fo by applyng e bounday condon () nβ n n, n, e and e (8) Ealuang () fo dffeen alue of e oban :,,, 5,, :,,, 5,, :,,, 5,, :,,,, 5, 5, n n,n n,n n 5,n n, n n n:, n n,n n,n n 5,n n, n n (9) Tu e yem of equaon (9) epeen n equaon n n unknon. Hence e eque o moe equaon c ae obaned fom e bounday condon e en e ae and e, and n n n n () e e Wee,, e e n and n Expeng e equaon (9)-() n max fom a A X B () ee e mace A, X and B ae gen n e appendx. B conan and n c ae e alue of on e bounday and X con of alue of n e egon. olng e yem () e ge e oluon fo Type B oluon fo eloce and We ake e follong bounday condon ( ) coβ n, n, ( ) d d ( ) d d d and d Ung e bounday condon ( ) d and ( ), e ge d And n n n () Fom (9) ubung,,..n, n and fom (), ng n max e ge a A X B () ee A, B ae gen n appendx. n n : 55
6 VOL. 5, NO. 5, MAY IN ARPN Jounal of Engneeng and Appled cence 6- Aan Reeac Publng Neok (ARPN). All g eeed..apnjounal.com mlaly e ue e follong bounday condon fo elocy a () nb n n, n, σ and Ung e condon σ and, e ge σ and () n n Fom () ubung,,..n, n and fom (), ng n max e ge a A X B (5) ee A and B ae gen n e appendx. On olng (5), e ge e oluon fo X, e alue of axal elocy. 5. DRAG ON THE CYLINDER Te dag D acng on a cylnde of leng L gen by D L π a ( T co β T n β ) d θ (6) Te e componen n (6) and Couple e eno M ae defned by e follong conue equaon fo couple e flud (oke []). T j PI λ ( Q ) I T µ ( Q ( Q ) ) I ( M ) ( Q ) η [ ( Q )] (7) T M mi η (8) Te e componen T and T on e cylnde can be calculaed a µq T e a (9) µq σ T e a () Applyng e fne dffeence ceme fo (9) and (), e non-dmenonal fom of e componen ae calculaed a σ T T µq a e σ σ µq e a Te non-dmenonal dag can be calculaed fom (6) a T n D () Wee co β T β D D Lπµ q 6. REULT AND DICUION Te analycal expeon fo e nondmenonal elocy componen, and dag ae gen by e equaon (), () and () epecely. Tee alue depend on e alue of β, f β, e ge only oonal ocllaon and f β π/, e ge only axal (Longudnal) ocllaon. Te numecal eul ae peened n e fom of gap fo, Re., σ.5, σ.5, β.7, n.6, π. Te Fgue fo ype A bounday condon ae on on lef column and e Fgue fo ype B condon ae on e g column. Te eloce and a dffeen Reynold numbe ype A and ype B bounday condon ae on n Fgue -5. We noce a a Reynold numbe Re nceae bo e eloce and deceae. Te eloce and a dffeen nondmenonal me ae on n Fgue 6-9. We obee a e anee and axal elocy componen nea e cylnde ae deelopng and flucuang aound zeo e ame fequency a e cylnde. A e a of a cycle, e flo a maxmum eloce locaed a e uface of cylnde, a gadual deceae oad zeo n e egon aay fom e cylnde. A e cycle connue, e eloce deceae e maxmum alue no longe a e cylnde uface bu nde e flo feld. Fom Fgue -, e ee a a e couple e paamee nceae, e anee elocy deceae fo ype A condon and nceae fo ype B condon and e axal elocy nceae fo ype A condon, le deceae fo ype B condon. Type B bounday condon doen nole e paamee e, c e ao of couple e coy coeffcen η and η'. In 56
7 VOL. 5, NO. 5, MAY IN ARPN Jounal of Engneeng and Appled cence 6- Aan Reeac Publng Neok (ARPN). All g eeed..apnjounal.com ype A condon, a can be een fom Fgue -5 bo e axal and anee eloce ae ngnfcan e. Te non-dmenonal dag calculaed numecally fo dffeen alue of non-dmenonal me n mulple of π/σ a fxed alue of σ, σ and e eul ae on n e Fgue 6-7. In e equaon of moon, local acceleaon em domnae f σ, σ ae lage. To ae all em of LH n e ame ode n equaon (9) and (), e fequency paamee σ, σ ae o be mall. Hence e ake bo σ, σ <. In e calculaon of dag alo e obee a f σ <, σ <, e dag ll be n eaonable alue. Fom Fgue 6-7, can be een a a e couple e paamee nceae, e amplude of ocllaon fo dag nceae fo bo e ype A and ype B condon. I can be een fo bo e ype A and ype B condon a σ nceae, e aaon n dag a e cylnde all ae cangng n amplude and fequency (Fgue 8-9). Fom Fgue- and Fgue-, obeed a e dag ngnfcan o e aaon n σ fo ype a condon and fo ype B condon e dag ocllae egulaly a σ nceae. Fom Fgue -, e noe a a Reynold numbe Re nceae magnude of dag nceae fo mall alue of ucon; bu fo ge alue of ucon dag nceae fo mall alue of Reynold numbe and en deceae a ge alue and almo conan fo ey g alue of ucon ae. Fom Fgue-, e noe a dag ngnfcan o e aaon n e, fo ype a condon and ype B condon ndependen of e. Fgue-. Type B aaon of. Fgue-. Type A aaon of. 7. CONCLUION We ae obeed a:. Te flo ene epec o couple e paamee and ype A and ype B condon o oppoe end..e., e anee elocy deceae fo ype A condon, nceae fo ype B condon;. Te dag nceae a nceae.e. e dag offeed by cou flud le an a of couple e flud; and. ucon on e cylnde deceae e dag. Fgue-5. Type B aaon of. Fgue-. Type A aaon of. 57
8 VOL. 5, NO. 5, MAY IN ARPN Jounal of Engneeng and Appled cence 6- Aan Reeac Publng Neok (ARPN). All g eeed..apnjounal.com Fgue-6. Type A aaon of Exp(σ ). Fgue-9. Type B aaon of Exp (σ ) Fgue-. Type A aaon of. Fgue-7. Type B aaon of Exp (σ ). Fgue-. Type B aaon of. Fgue-8. Type A aaon of Exp (σ ). 58
9 VOL. 5, NO. 5, MAY IN ARPN Jounal of Engneeng and Appled cence 6- Aan Reeac Publng Neok (ARPN). All g eeed..apnjounal.com Fgue-. Type A aaon of. Fgue-5. Type A aaon of. Fgue-. Type B aaon of. Fgue-6. Type A aaon of D' σ. Fgue-. Type A aaon of. Fgue-7. Type B aaon of D' σ. 59
10 VOL. 5, NO. 5, MAY IN ARPN Jounal of Engneeng and Appled cence 6- Aan Reeac Publng Neok (ARPN). All g eeed..apnjounal.com Fgue-8. Type A aaon of D'. Fgue-. Type B aaon of D'. Fgue-9. Type B aaon of D'. Fgue-. Type A aaon of D' Re. Fgue-. Type A aaon of D'. Fgue-. Type B aaon of D' Re. 6
11 VOL. 5, NO. 5, MAY IN ARPN Jounal of Engneeng and Appled cence 6- Aan Reeac Publng Neok (ARPN). All g eeed..apnjounal.com [] A.. Beman. 95. Lamna flo n cannel poou all. J. App. Py. : -5. [] J.R. ella Lamna flo n cannel poou all a g ucon Reynold numbe. J. Appl. Py. 6: [].W. Yuan Fue negaon of lamna flo n cannel poou all. J. Appl. Py. 7: REFERENCE Fgue-. Type A aaon of D'. [] V.K. oke Couple e n flud. Py. Flud. 9: [] V.K. oke. 98. Teoe of Flud Mcoucue. pnge, Ne Yok. [] G.G. oke On e effec of oaon of cylnde and pee abou e on axe n nceang e logamc decemen of e ac of baon. Cambdge Uney Pe, England. pp. 7-. [] M.J. Caaella and P.A. Laua Dag on ocllang od longudnal and oonal Moon. J. Hydonau. : 8-8. [5] K.R. Rajagopal. 98. Longudnal and Toonal ocllaon of a od n a non-neonan flud. Aca. Mec. 9: [6] H. Ramkoon and.r.majumda. 99. Flo due o e longudnal and onal ocllaon of a cylnde. ZAMP. : [7] H. Ramkoon, C.V. Eaaan and.r. Majumda. 99. Longudnal and Toonal ocllaon of a od n a pola flud. In. J. Engng. c. 9(): 5-. [8] C. Calmele-Eluu and D.R. Mazumda Flo of Mcopola flud oug a ccula cylnde ubjec o longudnal and onal ocllaon. Mal. Compu. Modelng. 7: [9] D. Oen and K. Raaman. 6. On e flo of an Oldoyd-B lqud oug a ag ccula ube pefomng longudnal and oonal ocllaon of dffeen fequence. Maemaca. : -9. [] R.M. Tel, G.M. ea Lamna flo oug paallel and unfomly poou all of dffeen pemeably. ZAMP. 6: 7-8. [] V. M. oundalgeka and R. N. Aanake. 97. Effec of couple ee on e ocllaoy flo pa an nfne plae conan ucon. Meccanca. pp [5] N. T. M. Eldabe, A. A. Haan and Mona A. A. Moamed.. Effec of Couple ee on e MHD of a Non-Neonan Uneady Flo beeen To Paallel Poou Plae. Z. Naufoc. 58a. -. [6] M. Deaka, T.K.V. Iyenga. 8. oke Poblem fo an Incompeble Couple e Flud. Nonlnea Analy: Modelng and Conol. (): 8-9. [7] D. naacaya, N. naacayulu, O. Odelu. 9. Flo and ea anfe of couple e flud n a poou cannel expandng and conacng all. Inenaonal Communcaon n Hea and Ma Tanfe. 6: [8] J.V. Ramana Muy and N.K. Baal. 9. eady flo of mcopola flud oug a ccula ppe unde a anee magnec feld conan ucon/njecon. In. J. of Appl. Ma and Mec. 5(): -. [9] P. Muu, B.V. Ra Kuma and Peeyu Canda. 8. Pealc moon of mcopola flud n cylndcal ube: effec of all popee. Appl. Ma. Modelng. : 9-. Appendx Te mace A, X, B ; A, X, B ; A, B and A, B defned eale n e equaon (7), (), () and (5) ae gen by e follong expeon. Te coeffcen max A gen n (7) defned a: 6
12 VOL. 5, NO. 5, MAY IN ARPN Jounal of Engneeng and Appled cence 6- Aan Reeac Publng Neok (ARPN). All g eeed..apnjounal.com, A,,,,,, 5,,,, 5,,, 5,, 5,,n,n,n,n,n,n,n,n,n,n 5,n,n,n,n 5,n,n 5 5,n Te oluon eco X fo elocy a dffeen pon gen by X [,,,,,. n 5, n, n, n, n, n, n, n ] T and e eco B fo e bounday alue gen by B [,,,,,,,..., 5, n n,, n n,, n n, 6 n ] T Te mace A, X, B defned n equaon () ae a follo. Te coeffcen max A gen by, A,,,,,, 5,,,, 5,,, 5,, 5,,n,n,n,n,n,n,n,n,n,n 5,n,n,n,n 5,n,n 5,n Te oluon eco X fo elocy a dffeen pon gen by X [,,,,,, 5.. n 5, n, n, n, n, n, n, n ] T and e eco B fo e bounday alue gen by B [,,,,,,,, 5, n n,, n n,, n n, n n ] T Te coeffcen max A defned n equaon () gen by 6
13 VOL. 5, NO. 5, MAY IN ARPN Jounal of Engneeng and Appled cence 6- Aan Reeac Publng Neok (ARPN). All g eeed..apnjounal.com, A,,,,,, 5,,,, 5,,, 5,, 5,,n,n,n,n,n,n,n,n,n,n 5,n,n,n,n 5,n,n 5,n and e eco B fo e bounday alue gen by B [(/ ),,,,,,,,.,, 5,n n,,n n,,n n, (/ n ) n ] T Te coeffcen max A defned n equaon (5) gen by, A,,,,,, 5,,,, 5,,, 5,, 5,,n,n,n,n,n,n,n,n,n,n 5,n,n,n,n 5,n,n 5,n and e eco B fo e bounday alue gen by B [σ,,,,,,,,.,, 5,n n,,n n,,n n,] T 6
CHAPTER 10: LINEAR DISCRIMINATION
HAPER : LINEAR DISRIMINAION Dscmnan-based lassfcaon 3 In classfcaon h K classes ( k ) We defned dsmnan funcon g () = K hen gven an es eample e chose (pedced) s class label as f g () as he mamum among g
More informationField due to a collection of N discrete point charges: r is in the direction from
Physcs 46 Fomula Shee Exam Coulomb s Law qq Felec = k ˆ (Fo example, f F s he elecc foce ha q exes on q, hen ˆ s a un veco n he decon fom q o q.) Elecc Feld elaed o he elecc foce by: Felec = qe (elecc
More informationESS 265 Spring Quarter 2005 Kinetic Simulations
SS 65 Spng Quae 5 Knec Sulaon Lecue une 9 5 An aple of an lecoagnec Pacle Code A an eaple of a knec ulaon we wll ue a one denonal elecoagnec ulaon code called KMPO deeloped b Yohhau Oua and Hoh Mauoo.
More informationCourse Outline. 1. MATLAB tutorial 2. Motion of systems that can be idealized as particles
Couse Oulne. MATLAB uoal. Moon of syses ha can be dealzed as pacles Descpon of oon, coodnae syses; Newon s laws; Calculang foces equed o nduce pescbed oon; Deng and solng equaons of oon 3. Conseaon laws
More informationOutline. GW approximation. Electrons in solids. The Green Function. Total energy---well solved Single particle excitation---under developing
Peenaon fo Theoecal Condened Mae Phyc n TU Beln Geen-Funcon and GW appoxmaon Xnzheng L Theoy Depamen FHI May.8h 2005 Elecon n old Oulne Toal enegy---well olved Sngle pacle excaon---unde developng The Geen
More information2 shear strain / L for small angle
Sac quaons F F M al Sess omal sess foce coss-seconal aea eage Shea Sess shea sess shea foce coss-seconal aea llowable Sess Faco of Safe F. S San falue Shea San falue san change n lengh ognal lengh Hooke
More informationChapter 6 Plane Motion of Rigid Bodies
Chpe 6 Pne oon of Rd ode 6. Equon of oon fo Rd bod. 6., 6., 6.3 Conde d bod ced upon b ee een foce,, 3,. We cn ume h he bod mde of e numbe n of pce of m Δm (,,, n). Conden f he moon of he m cene of he
More informationChapter 3: Vectors and Two-Dimensional Motion
Chape 3: Vecos and Two-Dmensonal Moon Vecos: magnude and decon Negae o a eco: eese s decon Mulplng o ddng a eco b a scala Vecos n he same decon (eaed lke numbes) Geneal Veco Addon: Tangle mehod o addon
More informations = rθ Chapter 10: Rotation 10.1: What is physics?
Chape : oaon Angula poson, velocy, acceleaon Consan angula acceleaon Angula and lnea quanes oaonal knec enegy oaonal nea Toque Newon s nd law o oaon Wok and oaonal knec enegy.: Wha s physcs? In pevous
More informationSUPERSONIC INVISCID FLOWS WITH THREE-DIMENSIONAL INTERACTION OF SHOCK WAVES IN CORNERS FORMED BY INTERSECTING WEDGES Y.P.
SUPERSONIC INVISCID FLOWS WITH THREE-DIMENSIONAL INTERACTION OF SHOCK WAVES IN CORNERS FORMED BY INTERSECTING WEDGES Y.P. Goonko, A.N. Kudyavev, and R.D. Rakhmov Inue of Theoecal and Appled Mechanc SB
More information5-1. We apply Newton s second law (specifically, Eq. 5-2). F = ma = ma sin 20.0 = 1.0 kg 2.00 m/s sin 20.0 = 0.684N. ( ) ( )
5-1. We apply Newon s second law (specfcally, Eq. 5-). (a) We fnd he componen of he foce s ( ) ( ) F = ma = ma cos 0.0 = 1.00kg.00m/s cos 0.0 = 1.88N. (b) The y componen of he foce s ( ) ( ) F = ma = ma
More informationNumerical Study of Large-area Anti-Resonant Reflecting Optical Waveguide (ARROW) Vertical-Cavity Semiconductor Optical Amplifiers (VCSOAs)
USOD 005 uecal Sudy of Lage-aea An-Reonan Reflecng Opcal Wavegude (ARROW Vecal-Cavy Seconduco Opcal Aplfe (VCSOA anhu Chen Su Fung Yu School of Eleccal and Eleconc Engneeng Conen Inoducon Vecal Cavy Seconduco
More informationAn Approach to the Representation of Gradual Uncertainty Resolution in Stochastic Multiperiod Planning
9 h Euopean mpoum on Compue Aded oce Engneeng ECAE9 J. Jeow and J. hulle (Edo 009 Eleve B.V./Ld. All gh eeved. An Appoach o he epeenaon of Gadual Uncean eoluon n ochac ulpeod lannng Vcene co-amez a gnaco
More informationajanuary't I11 F or,'.
',f,". ; q - c. ^. L.+T,..LJ.\ ; - ~,.,.,.,,,E k }."...,'s Y l.+ : '. " = /.. :4.,Y., _.,,. "-.. - '// ' 7< s k," ;< - " fn 07 265.-.-,... - ma/ \/ e 3 p~~f v-acecu ean d a e.eng nee ng sn ~yoo y namcs
More informationCptS 570 Machine Learning School of EECS Washington State University. CptS Machine Learning 1
ps 57 Machne Leann School of EES Washnon Sae Unves ps 57 - Machne Leann Assume nsances of classes ae lneal sepaable Esmae paamees of lnea dscmnan If ( - -) > hen + Else - ps 57 - Machne Leann lassfcaon
More informationMaximum Likelihood Estimation
Mau Lkelhood aon Beln Chen Depaen of Copue Scence & Infoaon ngneeng aonal Tawan oal Unvey Refeence:. he Alpaydn, Inoducon o Machne Leanng, Chape 4, MIT Pe, 4 Saple Sac and Populaon Paaee A Scheac Depcon
More informationCooling of a hot metal forging. , dt dt
Tranen Conducon Uneady Analy - Lumped Thermal Capacy Model Performed when; Hea ranfer whn a yem produced a unform emperaure drbuon n he yem (mall emperaure graden). The emperaure change whn he yem condered
More informationL4:4. motion from the accelerometer. to recover the simple flutter. Later, we will work out how. readings L4:3
elave moon L4:1 To appl Newon's laws we need measuemens made fom a 'fed,' neal efeence fame (unacceleaed, non-oang) n man applcaons, measuemens ae made moe smpl fom movng efeence fames We hen need a wa
More informationPHY2053 Summer C 2013 Exam 1 Solutions
PHY053 Sue C 03 E Soluon. The foce G on o G G The onl cobnon h e '/ = doubln.. The peed of lh le 8fulon c 86,8 le 60 n 60n h 4h d 4d fonh.80 fulon/ fonh 3. The dnce eled fo he ene p,, 36 (75n h 45 The
More informationSkin Effect and Formation Damage
Well Stimulation and Sand Poduction Management (PGE 489 ) Sin Effect and Fomation Damage By D. Moammed A. Kami 02-02-2016 Sin Facto A fomation damage model i a dynamic elationip expeing te fluid tanpot
More informationName of the Student:
Engneeng Mahemacs 05 SUBJEC NAME : Pobably & Random Pocess SUBJEC CODE : MA645 MAERIAL NAME : Fomula Maeal MAERIAL CODE : JM08AM007 REGULAION : R03 UPDAED ON : Febuay 05 (Scan he above QR code fo he dec
More informationExercise 4: Adimensional form and Rankine vortex. Example 1: adimensional form of governing equations
Fluid Mechanics, SG4, HT9 Septembe, 9 Execise 4: Adimensional fom and Rankine votex Example : adimensional fom of govening equations Calculating the two-dimensional flow aound a cylinde (adius a, located
More informationA PATRA CONFERINŢĂ A HIDROENERGETICIENILOR DIN ROMÂNIA,
A PATRA ONFERINŢĂ A HIDROENERGETIIENILOR DIN ROMÂNIA, Do Pael MODELLING OF SEDIMENTATION PROESS IN LONGITUDINAL HORIZONTAL TANK MODELAREA PROESELOR DE SEPARARE A FAZELOR ÎN DEANTOARE LONGITUDINALE Da ROBESU,
More informationInformation Fusion Kalman Smoother for Time-Varying Systems
Infoaon Fuon alan oohe fo Te-Vayng ye Xao-Jun un Z- Deng Abac-- Fo he lnea dcee e-ayng ochac conol ye wh uleno coloed eaueen noe hee dbued opal fuon alan oohe ae peened baed on he opal nfoaon fuon ule
More informationModern Energy Functional for Nuclei and Nuclear Matter. By: Alberto Hinojosa, Texas A&M University REU Cyclotron 2008 Mentor: Dr.
Moden Enegy Funconal fo Nucle and Nuclea Mae By: lbeo noosa Teas &M Unvesy REU Cycloon 008 Meno: D. Shalom Shlomo Oulne. Inoducon.. The many-body poblem and he aee-fock mehod. 3. Skyme neacon. 4. aee-fock
More informationA multiple-relaxation-time lattice Boltzmann model for simulating. incompressible axisymmetric thermal flows in porous media
A mulple-elaxaon-me lace Bolmann model fo smulang ncompessble axsymmec hemal flows n poous meda Qng Lu a, Ya-Lng He a, Qng L b a Key Laboaoy of Themo-Flud Scence and Engneeng of Mnsy of Educaon, School
More informationLecture 5. Plane Wave Reflection and Transmission
Lecue 5 Plane Wave Reflecon and Tansmsson Incden wave: 1z E ( z) xˆ E (0) e 1 H ( z) yˆ E (0) e 1 Nomal Incdence (Revew) z 1 (,, ) E H S y (,, ) 1 1 1 Refleced wave: 1z E ( z) xˆ E E (0) e S H 1 1z H (
More informationAn axisymmetric incompressible lattice BGK model for simulation of the pulsatile ow in a circular pipe
INTERNATIONAL JOURNAL FOR NUMERICAL METHODS IN FLUIDS In. J. Nume. Meh. Fluds 005; 49:99 116 Publshed onlne 3 June 005 n Wley IneScence www.nescence.wley.com). DOI: 10.100/d.997 An axsymmec ncompessble
More information( ) ( ) ( ) ( ) ( ) ( ) j ( ) A. b) Theorem
b) Theoe The u of he eco pojecon of eco n ll uull pependcul (n he ene of he cl poduc) decon equl o he eco. ( ) n e e o The pojecon conue he eco coponen of he eco. poof. n e ( ) ( ) ( ) e e e e e e e e
More informationOverview. Overview Page 1 of 8
COMPUTERS AND STRUCTURES, INC., BERKELEY, CALIORNIA DECEMBER 2001 COMPOSITE BEAM DESIGN AISC-LRD93 Tecnical Noe Compac and Noncompac Requiemens Tis Tecnical Noe descibes o e pogam cecks e AISC-LRD93 specificaion
More informationMultiple Batch Sizing through Batch Size Smoothing
Jounal of Indual Engneeng (9)-7 Mulple Bach Szng hough Bach Sze Smoohng M Bahadoghol Ayanezhad a, Mehd Kam-Naab a,*, Sudabeh Bakhh a a Depamen of Indual Engneeng, Ian Unvey of Scence and Technology, Tehan,
More informationOptimal control of Goursat-Darboux systems in domains with curvilinear boundaries
Opmal conol of Goua-Daboux yem n doman wh cuvlnea boundae S. A. Belba Mahemac Depamen Unvey of Alabama Tucalooa, AL. 35487-0350. USA. e-mal: SBELBAS@G.AS.UA.EDU Abac. We deve neceay condon fo opmaly n
More informationSCIENCE CHINA Technological Sciences
SIENE HINA Technologcal Scences Acle Apl 4 Vol.57 No.4: 84 8 do:.7/s43-3-5448- The andom walkng mehod fo he seady lnea convecondffuson equaon wh axsymmec dsc bounday HEN Ka, SONG MengXuan & ZHANG Xng *
More informationWater Tunnel Experiment MAE 171A/175A. Objective:
Wate Tunnel Expeiment MAE 7A/75A Objective: Measuement of te Dag Coefficient of a Cylinde Measuement Tecniques Pessue Distibution on Cylinde Dag fom Momentum Loss Measued in Wake it lase Dopple Velocimety
More informationRotor Power Feedback Control of Wind Turbine System with Doubly-Fed Induction Generator
Poceedn of he 6h WSEAS Inenaonal Confeence on Smulaon Modelln and Opmzaon Lbon Poual Sepembe -4 6 48 Roo Powe Feedback Conol of Wnd Tubne Syem wh Doubly-Fed Inducon Geneao J. Smajo Faculy of Eleccal Enneen
More informationVehicle Suspension Inspection by Stewart Robot
Vehcle Supenon Inpecon by Sewa Robo.Kazem 1,* and. Joohan 2 Downloaded fom www.u.ac. a 4:7 IRST on Wedneday Januay 23d 219 1 an Pofeo,Depamen of Eleccal Engneeng,Shahed Unvey, Tehan, Ian.2 c Suden Eleccal
More informationN 1. Time points are determined by the
upplemena Mehods Geneaon of scan sgnals In hs secon we descbe n deal how scan sgnals fo 3D scannng wee geneaed. can geneaon was done n hee seps: Fs, he dve sgnal fo he peo-focusng elemen was geneaed o
More informationH = d d q 1 d d q N d d p 1 d d p N exp
8333: Sacal Mechanc I roblem Se # 7 Soluon Fall 3 Canoncal Enemble Non-harmonc Ga: The Hamlonan for a ga of N non neracng parcle n a d dmenonal box ha he form H A p a The paron funcon gven by ZN T d d
More informationGo over vector and vector algebra Displacement and position in 2-D Average and instantaneous velocity in 2-D Average and instantaneous acceleration
Mh Csquee Go oe eco nd eco lgeb Dsplcemen nd poson n -D Aege nd nsnneous eloc n -D Aege nd nsnneous cceleon n -D Poecle moon Unfom ccle moon Rele eloc* The componens e he legs of he gh ngle whose hpoenuse
More informationRotational Kinematics. Rigid Object about a Fixed Axis Western HS AP Physics 1
Rotatonal Knematcs Rgd Object about a Fxed Axs Westen HS AP Physcs 1 Leanng Objectes What we know Unfom Ccula Moton q s Centpetal Acceleaton : Centpetal Foce: Non-unfom a F c c m F F F t m ma t What we
More informationFast Calibration for Robot Welding System with Laser Vision
Fas Calbaon fo Robo Weldng Ssem h Lase Vson Lu Su Mechancal & Eleccal Engneeng Nanchang Unves Nanchang, Chna Wang Guoong Mechancal Engneeng Souh Chna Unves of echnolog Guanghou, Chna Absac Camea calbaon
More informationMATRIX COMPUTATIONS ON PROJECTIVE MODULES USING NONCOMMUTATIVE GRÖBNER BASES
Jounal of lgeba Numbe heo: dance and pplcaon Volume 5 Numbe 6 Page -9 alable a hp://cenfcadance.co.n DOI: hp://d.do.og/.86/janaa_7686 MRIX COMPUIONS ON PROJCIV MODULS USING NONCOMMUIV GRÖBNR BSS CLUDI
More informationNote: Please use the actual date you accessed this material in your citation.
MIT OpenCuseWae hp://cw.m.edu 6.03/ESD.03J Elecmagnecs and Applcans, Fall 005 Please use he fllwng can fma: Makus Zahn, Ech Ippen, and Davd Saeln, 6.03/ESD.03J Elecmagnecs and Applcans, Fall 005. (Massachuses
More informationPhys 2310 Fri. Oct. 23, 2017 Today s Topics. Begin Chapter 6: More on Geometric Optics Reading for Next Time
Py F. Oct., 7 Today Topc Beg Capte 6: Moe o Geometc Optc eadg fo Next Tme Homewok t Week HW # Homewok t week due Mo., Oct. : Capte 4: #47, 57, 59, 6, 6, 6, 6, 67, 7 Supplemetal: Tck ee ad e Sytem Pcple
More informationMolecular Evolution and Phylogeny. Based on: Durbin et al Chapter 8
Molecula Evoluion and hylogeny Baed on: Dubin e al Chape 8. hylogeneic Tee umpion banch inenal node leaf Topology T : bifucaing Leave - N Inenal node N+ N- Lengh { i } fo each banch hylogeneic ee Topology
More informationFlow Decomposition and Large Deviations
ounal of funconal analy 14 2367 (1995) acle no. 97 Flow Decompoon and Lage Devaon Ge ad Ben Aou and Fabenne Caell Laboaoe de Mode laon ochaque e aque Unvee Pa-Sud (Ba^. 425) 91-45 Oay Cedex Fance Receved
More informationTransient Thermal Stress Prediction Due To Flow of Coolant Through Hot Pipe
Eng. & Tech. Jounal Vol. 9, No., Tansen Themal Sess Pedcon Due To Flow of Coolan Though Ho Ppe D. Jalal M. Jall* & Receved on: // Acceped on: // Anes F. Saad* Absac Tansen hemal sesses n ppe wall due o
More informationLattice-Boltzmann model for axisymmetric thermal flows
Lace-Bolzmann model fo asymmec hemal flows Q. L, Y. L. He, G. H. Tan, and W. Q. Tao Naonal Key Laboaoy of Mulphase Flow n Powe Enneen, School of Eney and Powe Enneen, X an Jaoon Unvesy, X an, Shaan 71009,
More informationMass-Spring Systems Surface Reconstruction
Mass-Spng Syses Physally-Based Modelng: Mass-Spng Syses M. Ale O. Vasles Mass-Spng Syses Mass-Spng Syses Snake pleenaon: Snake pleenaon: Iage Poessng / Sae Reonson: Iage poessng/ Sae Reonson: Mass-Spng
More informationChapter 13 - Universal Gravitation
Chapte 3 - Unesal Gataton In Chapte 5 we studed Newton s thee laws of moton. In addton to these laws, Newton fomulated the law of unesal gataton. Ths law states that two masses ae attacted by a foce gen
More informationCopula Effect on Scenario Tree
IAENG Inenaonal Jounal of Appled Mahemac 37: IJAM_37 8 Copula Effec on Scenao Tee K. Suene and H. Panevcu Abac Mulage ochac pogam ae effecve fo olvng long-em plannng poblem unde unceany. Such pogam ae
More informationFall 2004/05 Solutions to Assignment 5: The Stationary Phase Method Provided by Mustafa Sabri Kilic. I(x) = e ixt e it5 /5 dt (1) Z J(λ) =
8.35 Fall 24/5 Solution to Aignment 5: The Stationay Phae Method Povided by Mutafa Sabi Kilic. Find the leading tem fo each of the integal below fo λ >>. (a) R eiλt3 dt (b) R e iλt2 dt (c) R eiλ co t dt
More informationMotion in Two Dimensions
Phys 1 Chaper 4 Moon n Two Dmensons adzyubenko@csub.edu hp://www.csub.edu/~adzyubenko 005, 014 A. Dzyubenko 004 Brooks/Cole 1 Dsplacemen as a Vecor The poson of an objec s descrbed by s poson ecor, r The
More informationChapter Finite Difference Method for Ordinary Differential Equations
Chape 8.7 Fne Dffeence Mehod fo Odnay Dffeenal Eqaons Afe eadng hs chape, yo shold be able o. Undesand wha he fne dffeence mehod s and how o se o solve poblems. Wha s he fne dffeence mehod? The fne dffeence
More informationPhysics 120 Spring 2007 Exam #1 April 20, Name
Phc 0 Spng 007 E # pl 0, 007 Ne P Mulple Choce / 0 Poble # / 0 Poble # / 0 Poble # / 0 ol / 00 In eepng wh he Unon College polc on cdec hone, ued h ou wll nehe ccep no pode unuhozed nce n he copleon o
More informationdm dt = 1 V The number of moles in any volume is M = CV, where C = concentration in M/L V = liters. dcv v
Mg: Pcess Aalyss: Reac ae s defed as whee eac ae elcy lue M les ( ccea) e. dm he ube f les ay lue s M, whee ccea M/L les. he he eac ae beces f a hgeeus eac, ( ) d Usually s csa aqueus eeal pcesses eac,
More informationNanoparticles. Educts. Nucleus formation. Nucleus. Growth. Primary particle. Agglomeration Deagglomeration. Agglomerate
ucs Nucleus Nucleus omaon cal supesauaon Mng o eucs, empeaue, ec. Pmay pacle Gowh Inegaon o uson-lme pacle gowh Nanopacles Agglomeaon eagglomeaon Agglomeae Sablsaon o he nanopacles agans agglomeaon! anspo
More informationParametric Instability Investigation and Stability Based Design for Transmission Systems Containing Face-gear Drives
Unvey of Tenneee, Knoxvlle Tace: Tenneee Reeach and Ceave Exchange Docoal Deaon Gaduae School 8- Paamec Inably Invegaon and Sably Baed Degn fo Tanmon Syem Conanng Face-gea Dve Meng Peng mpeng@u.edu Recommended
More information1 Constant Real Rate C 1
Consan Real Rae. Real Rae of Inees Suppose you ae equally happy wh uns of he consumpon good oday o 5 uns of he consumpon good n peod s me. C 5 Tha means you ll be pepaed o gve up uns oday n eun fo 5 uns
More information24-2: Electric Potential Energy. 24-1: What is physics
D. Iyad SAADEDDIN Chapte 4: Electc Potental Electc potental Enegy and Electc potental Calculatng the E-potental fom E-feld fo dffeent chage dstbutons Calculatng the E-feld fom E-potental Potental of a
More informationLOW ORDER POLYNOMIAL EXPANSION NODAL METHOD FOR A DeCART AXIAL SOLUTION
9 Inenaona Nucea Aanc Confeence - INAC 9 Ro de JaneoRJ az epembe7 o Ocobe 9 AOCIAÇÃO RAILEIRA DE ENERGIA NUCLEAR - AEN IN: 978-85-994--8 LOW ORDER POLYNOMIAL EXPANION NODAL METHOD FOR A DeCART AXIAL OLUTION
More informationThe Feigel Process. The Momentum of Quantum Vacuum. Geert Rikken Vojislav Krstic. CNRS-France. Ariadne call A0/1-4532/03/NL/MV 04/1201
The Fegel Pocess The Momenum of Quanum Vacuum a an Tggelen CNRS -Fance Laboaoe e Physque e Moélsaon es Mleux Complexes Unesé Joseph Foue/CNRS, Genoble, Fance Gee Ren Vosla Ksc CNRS Fance CNRS-Fance Laboaoe
More informationControl Systems. Mathematical Modeling of Control Systems.
Conrol Syem Mahemacal Modelng of Conrol Syem chbum@eoulech.ac.kr Oulne Mahemacal model and model ype. Tranfer funcon model Syem pole and zero Chbum Lee -Seoulech Conrol Syem Mahemacal Model Model are key
More information(,,, ) (,,, ). In addition, there are three other consumers, -2, -1, and 0. Consumer -2 has the utility function
MACROECONOMIC THEORY T J KEHOE ECON 87 SPRING 5 PROBLEM SET # Conder an overlappng generaon economy le ha n queon 5 on problem e n whch conumer lve for perod The uly funcon of he conumer born n perod,
More informationBasic molecular dynamics
1.1, 3.1, 1.333,. Inoducon o Modelng and Smulaon Spng 11 Pa I Connuum and pacle mehods Basc molecula dynamcs Lecue Makus J. Buehle Laboaoy fo Aomsc and Molecula Mechancs Depamen of Cvl and Envonmenal Engneeng
More informationSolution of Non-homogeneous bulk arrival Two-node Tandem Queuing Model using Intervention Poisson distribution
Volume-03 Issue-09 Sepembe-08 ISSN: 455-3085 (Onlne) RESEARCH REVIEW Inenaonal Jounal of Muldscplnay www.jounals.com [UGC Lsed Jounal] Soluon of Non-homogeneous bulk aval Two-node Tandem Queung Model usng
More informationCOMPLEMENTARY ENERGY METHOD FOR CURVED COMPOSITE BEAMS
ultscence - XXX. mcocd Intenatonal ultdscplnay Scentfc Confeence Unvesty of skolc Hungay - pl 06 ISBN 978-963-358-3- COPLEENTRY ENERGY ETHOD FOR CURVED COPOSITE BES Ákos József Lengyel István Ecsed ssstant
More informationELEC 201 Electric Circuit Analysis I Lecture 9(a) RLC Circuits: Introduction
//6 All le courey of Dr. Gregory J. Mazzaro EE Elecrc rcu Analy I ecure 9(a) rcu: Inroucon THE ITADE, THE MIITAY OEGE OF SOUTH AOINA 7 Moulre Sree, harleon, S 949 V Sere rcu: Analog Dcoery _ 5 Ω pf eq
More informationGravity. David Barwacz 7778 Thornapple Bayou SE, Grand Rapids, MI David Barwacz 12/03/2003
avity David Bawacz 7778 Thonapple Bayou, and Rapid, MI 495 David Bawacz /3/3 http://membe.titon.net/daveb Uing the concept dicued in the peceding pape ( http://membe.titon.net/daveb ), I will now deive
More informationTest 2 phy a) How is the velocity of a particle defined? b) What is an inertial reference frame? c) Describe friction.
Tet phy 40 1. a) How i the velocity of a paticle defined? b) What i an inetial efeence fae? c) Decibe fiction. phyic dealt otly with falling bodie. d) Copae the acceleation of a paticle in efeence fae
More information2/20/2013. EE 101 Midterm 2 Review
//3 EE Mderm eew //3 Volage-mplfer Model The npu ressance s he equalen ressance see when lookng no he npu ermnals of he amplfer. o s he oupu ressance. I causes he oupu olage o decrease as he load ressance
More informationUniversal Gravitation
Chapte 1 Univesal Gavitation Pactice Poblem Solutions Student Textbook page 580 1. Conceptualize the Poblem - The law of univesal gavitation applies to this poblem. The gavitational foce, F g, between
More informationRotor profile design in a hypogerotor pump
Jounal of Mechancal Scence and Technology (009 459~470 Jounal of Mechancal Scence and Technology www.spngelnk.com/conen/78-494x DOI 0.007/s06-009-007-y oo pofle desgn n a hypogeoo pump Soon-Man Kwon *,
More informationScienceDirect. Behavior of Integral Curves of the Quasilinear Second Order Differential Equations. Alma Omerspahic *
Avalable onlne a wwwscencedeccom ScenceDec oceda Engneeng 69 4 85 86 4h DAAAM Inenaonal Smposum on Inellgen Manufacung and Auomaon Behavo of Inegal Cuves of he uaslnea Second Ode Dffeenal Equaons Alma
More informationone primary direction in which heat transfers (generally the smallest dimension) simple model good representation for solving engineering problems
CHAPTER 3: One-Dimenional Steady-State Conduction one pimay diection in which heat tanfe (geneally the mallet dimenion) imple model good epeentation fo olving engineeing poblem 3. Plane Wall 3.. hot fluid
More information176 5 t h Fl oo r. 337 P o ly me r Ma te ri al s
A g la di ou s F. L. 462 E l ec tr on ic D ev el op me nt A i ng er A.W.S. 371 C. A. M. A l ex an de r 236 A d mi ni st ra ti on R. H. (M rs ) A n dr ew s P. V. 326 O p ti ca l Tr an sm is si on A p ps
More informationCHAPTER II AC POWER CALCULATIONS
CHAE AC OWE CACUAON Conens nroducon nsananeous and Aerage ower Effece or M alue Apparen ower Coplex ower Conseraon of AC ower ower Facor and ower Facor Correcon Maxu Aerage ower ransfer Applcaons 3 nroducon
More informationChapter Fifiteen. Surfaces Revisited
Chapte Ffteen ufaces Revsted 15.1 Vecto Descpton of ufaces We look now at the vey specal case of functons : D R 3, whee D R s a nce subset of the plane. We suppose s a nce functon. As the pont ( s, t)
More informationTHIS PAGE DECLASSIFIED IAW EO IRIS u blic Record. Key I fo mation. Ma n: AIR MATERIEL COMM ND. Adm ni trative Mar ings.
T H S PA G E D E CLA SSFED AW E O 2958 RS u blc Recod Key fo maon Ma n AR MATEREL COMM ND D cumen Type Call N u b e 03 V 7 Rcvd Rel 98 / 0 ndexe D 38 Eneed Dae RS l umbe 0 0 4 2 3 5 6 C D QC d Dac A cesson
More informationP a g e 5 1 of R e p o r t P B 4 / 0 9
P a g e 5 1 of R e p o r t P B 4 / 0 9 J A R T a l s o c o n c l u d e d t h a t a l t h o u g h t h e i n t e n t o f N e l s o n s r e h a b i l i t a t i o n p l a n i s t o e n h a n c e c o n n e
More informationA hybrid method to find cumulative distribution function of completion time of GERT networks
Jounal of Indusal Engneeng Inenaonal Sepembe 2005, Vol., No., - 9 Islamc Azad Uvesy, Tehan Souh Banch A hybd mehod o fnd cumulave dsbuon funcon of compleon me of GERT newos S. S. Hashemn * Depamen of Indusal
More informationI-POLYA PROCESS AND APPLICATIONS Leda D. Minkova
The XIII Inenaonal Confeence Appled Sochasc Models and Daa Analyss (ASMDA-009) Jne 30-Jly 3, 009, Vlns, LITHUANIA ISBN 978-9955-8-463-5 L Sakalaskas, C Skadas and E K Zavadskas (Eds): ASMDA-009 Seleced
More informationSupport Vector Machines
Suppo Veco Machine CSL 3 ARIFICIAL INELLIGENCE SPRING 4 Suppo Veco Machine O, Kenel Machine Diciminan-baed mehod olean cla boundaie Suppo veco coni of eample cloe o bounday Kenel compue imilaiy beeen eample
More informationDo not turn over until you are told to do so by the Invigilator.
UNIVERSITY OF EAST ANGLIA School of Mathematics Main Seies UG Examination 2015 16 FLUID DYNAMICS WITH ADVANCED TOPICS MTH-MD59 Time allowed: 3 Hous Attempt QUESTIONS 1 and 2, and THREE othe questions.
More informationChapter 6. NEWTON S 2nd LAW AND UNIFORM CIRCULAR MOTION. string
Chapte 6 NEWTON S nd LAW AND UNIFORM CIRCULAR MOTION 103 PHYS 1 1 L:\103 Phy LECTURES SLIDES\103Phy_Slide_T1Y3839\CH6Flah 3 4 ting Quetion: A ball attached to the end of a ting i whiled in a hoizontal
More informationINDOOR CHANNEL MODELING AT 60 GHZ FOR WIRELESS LAN APPLICATIONS
IDOOR CHAEL MODELIG AT 60 GHZ FOR WIRELESS LA APPLICATIOS ekaos Moas, Plp Consannou aonal Tecncal Unesy of Aens, Moble RadoCommuncons Laboaoy 9 Heoon Polyecnou 15773 Zogafou, Aens, Geece, moa@moble.nua.g
More informationChapter 6. NEWTON S 2nd LAW AND UNIFORM CIRCULAR MOTION
Chapte 6 NEWTON S nd LAW AND UNIFORM CIRCULAR MOTION Phyic 1 1 3 4 ting Quetion: A ball attached to the end of a ting i whiled in a hoizontal plane. At the point indicated, the ting beak. Looking down
More informationDetection and Estimation Theory
ESE 54 Detecton and Etmaton Theoy Joeph A. O Sullvan Samuel C. Sach Pofeo Electonc Sytem and Sgnal Reeach Laboatoy Electcal and Sytem Engneeng Wahngton Unvety 411 Jolley Hall 314-935-4173 (Lnda anwe) jao@wutl.edu
More informationASTR 3740 Relativity & Cosmology Spring Answers to Problem Set 4.
ASTR 3740 Relativity & Comology Sping 019. Anwe to Poblem Set 4. 1. Tajectoie of paticle in the Schwazchild geomety The equation of motion fo a maive paticle feely falling in the Schwazchild geomety ae
More informationA 1. EN2210: Continuum Mechanics. Homework 7: Fluid Mechanics Solutions
EN10: Continuum Mechanics Homewok 7: Fluid Mechanics Solutions School of Engineeing Bown Univesity 1. An ideal fluid with mass density ρ flows with velocity v 0 though a cylindical tube with cosssectional
More information) from i = 0, instead of i = 1, we have =
Chape 3: Adjusmen Coss n he abou Make I Movaonal Quesons and Execses: Execse 3 (p 6): Illusae he devaon of equaon (35) of he exbook Soluon: The neempoal magnal poduc of labou s epesened by (3) = = E λ
More informationStability Analysis of a Sliding-Mode Speed Observer during Transient State
Poceedng of he 5h WA In. Conf. on Inuenaon Meaueen Ccu and ye Hangzhou Chna Apl 6-8 006 (pp35-40 ably Analy of a ldng-mode peed Obeve dung anen ae WIO ANGUNGONG AAWU UJIJON chool of leccal ngneeng Inue
More informationRecursive segmentation procedure based on the Akaike information criterion test
ecuve egmenaon pocedue baed on he Aae nfomaon ceon e A-Ho SAO Depamen of Appled Mahemac and Phyc Gaduae School of Infomac Kyoo Unvey a@.yoo-u.ac.jp JAPAN Oulne Bacgound and Movaon Segmenaon pocedue baed
More informationSimulation of Non-normal Autocorrelated Variables
Jounal of Moden Appled Sascal Mehods Volume 5 Issue Acle 5 --005 Smulaon of Non-nomal Auocoelaed Vaables HT Holgesson Jönöpng Inenaonal Busness School Sweden homasholgesson@bshse Follow hs and addonal
More informationA. Inventory model. Why are we interested in it? What do we really study in such cases.
Some general yem model.. Inenory model. Why are we nereed n? Wha do we really udy n uch cae. General raegy of machng wo dmlar procee, ay, machng a fa proce wh a low one. We need an nenory or a buffer or
More informationCOLLEGE OF FOUNDATION AND GENERAL STUDIES PUTRAJAYA CAMPUS FINAL EXAMINATION TRIMESTER /2017
COLLEGE OF FOUNDATION AND GENERAL STUDIES PUTRAJAYA CAMPUS FINAL EXAMINATION TRIMESTER 1 016/017 PROGRAMME SUBJECT CODE : Foundaton n Engneeng : PHYF115 SUBJECT : Phscs 1 DATE : Septembe 016 DURATION :
More informationChapter 5. Long Waves
ape 5. Lo Waes Wae e s o compaed ae dep: < < L π Fom ea ae eo o s s ; amos ozoa moo z p s ; dosac pesse Dep-aeaed coseao o mass
More informationStatic Electric Fields. Coulomb s Law Ε = 4πε. Gauss s Law. Electric Potential. Electrical Properties of Materials. Dielectrics. Capacitance E.
Coulomb Law Ε Gau Law Electic Potential E Electical Popetie of Mateial Conducto J σe ielectic Capacitance Rˆ V q 4πε R ρ v 2 Static Electic Field εe E.1 Intoduction Example: Electic field due to a chage
More informationMolecular dynamics modeling of thermal and mechanical properties
Molecula dynamcs modelng of hemal and mechancal popees Alejando Sachan School of Maeals Engneeng Pudue Unvesy sachan@pudue.edu Maeals a molecula scales Molecula maeals Ceamcs Meals Maeals popees chas Maeals
More informationUniversity of Illinois at Chicago Department of Physics. Electricity & Magnetism Qualifying Examination
E&M poblems Univesity of Illinois at Chicago Depatment of Physics Electicity & Magnetism Qualifying Examination Januay 3, 6 9. am : pm Full cedit can be achieved fom completely coect answes to 4 questions.
More information